<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">NS</journal-id><journal-title-group><journal-title>Natural Science</journal-title></journal-title-group><issn pub-type="epub">2150-4091</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ns.2016.83018</article-id><article-id pub-id-type="publisher-id">NS-64668</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Chemistry&amp;Materials Science</subject><subject> Earth&amp;Environmental Sciences</subject><subject> Medicine&amp;Healthcare</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Quantum Dark Energy from the Hyperbolic Transfinite Cantorian Geometry of the Cosmos
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ohamed</surname><given-names>S. El Naschie</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Physics, University of Alexandria, Alexandria, Egypt</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>07</day><month>03</month><year>2016</year></pub-date><volume>08</volume><issue>03</issue><fpage>152</fpage><lpage>159</lpage><history><date date-type="received"><day>25</day>	<month>February</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>14</month>	<year>March</year>	</date><date date-type="accepted"><day>17</day>	<month>March</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The quintessence of hyperbolic geometry is transferred to a transfinite Cantorian-fractal setting in the present work. Starting from the building block of E-infinity Cantorian spacetime theory, namely a quantum pre-particle zero set as a core and a quantum pre-wave empty set as cobordism or surface of the core, we connect the interaction of two such self similar units to a compact four dimensional manifold and a corresponding holographic boundary akin to the compactified Klein modular curve with SL(2,7) symmetry. Based on this model in conjunction with a 4D compact hy- perbolic manifold M(4) and the associated general theory, the so obtained ordinary and dark en- ergy density of the cosmos is found to be in complete agreement with previous analysis as well as cosmic measurements and observations such as WMAP and Type 1a supernova.
 
</p></abstract><kwd-group><kwd>Dark Energy</kwd><kwd> Accelerated Cosmic Expansion</kwd><kwd> Hyperbolic Geometry</kwd><kwd> Fractal Geometry</kwd><kwd> Transfinite set Theory</kwd><kwd> ‘tHooft Dimensional Regularization</kwd><kwd> Hardy’s Quantum Entanglement</kwd><kwd> Davis Hyperbolic Manifold</kwd><kwd> Compactified Klein Modular Curve</kwd><kwd> Fractal Counting</kwd><kwd> Lie Symmetry Groups</kwd><kwd> Stein Spaces</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction and Preliminary Information</title><p>The present work gives explicit analysis for determining the ordinary and the dark energy density of the universe [<xref ref-type="bibr" rid="scirp.64668-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref2">2</xref>] based on an unorthodox combination of modern extension of hyperbolic geometry [<xref ref-type="bibr" rid="scirp.64668-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref4">4</xref>] and recent advances in nonlinear dynamics, deterministic chaos and random fractals [<xref ref-type="bibr" rid="scirp.64668-ref5">5</xref>] . We start from two parallel lines of thinking, namely first from our topological conception of a pre-quantum particle described by a bi dimension</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x6.png" xlink:type="simple"/></inline-formula>zero set [<xref ref-type="bibr" rid="scirp.64668-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref7">7</xref>] and a pre-quantum wave modelled by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x7.png" xlink:type="simple"/></inline-formula> empty set [<xref ref-type="bibr" rid="scirp.64668-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref7">7</xref>] where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x8.png" xlink:type="simple"/></inline-formula> as found from the generic von Neumann-Connes dimensional function of an x manifold corresponding to Penrose fractal tiling universe [<xref ref-type="bibr" rid="scirp.64668-ref6">6</xref>]</p><disp-formula id="scirp.64668-formula28"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x9.png"  xlink:type="simple"/></disp-formula><p>The second line of thinking within the present scheme is the compact 4D hyperbolic manifold M<sup>(4)</sup> of M.W.</p><p>Davis [<xref ref-type="bibr" rid="scirp.64668-ref4">4</xref>] which has 1400 cells and a hyperbolic volume equal <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x10.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.64668-ref4">4</xref>] . Incidentally the Euler characteristic of this manifold is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x11.png" xlink:type="simple"/></inline-formula> which differs from that of E-infinity Cantorian spacetime [<xref ref-type="bibr" rid="scirp.64668-ref6">6</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref14">14</xref>] by only <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x12.png" xlink:type="simple"/></inline-formula> being <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x13.png" xlink:type="simple"/></inline-formula> where k is the ‘tHooft renormalon [<xref ref-type="bibr" rid="scirp.64668-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref15">15</xref>] . The possibility of a Hardy entangleon elementary particle <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x14.png" xlink:type="simple"/></inline-formula> as well as an entangleon particle <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x15.png" xlink:type="simple"/></inline-formula> was proposed by the</p><p>present Author as well as others a relatively short time ago [<xref ref-type="bibr" rid="scirp.64668-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref15">15</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref17">17</xref>] . From here onwards and as we will see momentarily, the two lines of though mentioned will converge towards a common conclusion, namely that the holographic boundary of our universe can be modelled exactly by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x16.png" xlink:type="simple"/></inline-formula> degrees of freedom of a compactified Klein modular curve plus gravity and spacetime [<xref ref-type="bibr" rid="scirp.64668-ref6">6</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref11">11</xref>] and that the exact ordinary energy density of the cosmos is given by [<xref ref-type="bibr" rid="scirp.64668-ref8">8</xref>]</p><disp-formula id="scirp.64668-formula29"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x17.png"  xlink:type="simple"/></disp-formula><p>where R<sup>(4)</sup> = 20 is the number of independent components of the Riemann-Einstein tensor in D<sup>(4)</sup> = 4 dimensional Einstein spacetime. Inserting in E(O) of equation (2) one finds the obvious result [<xref ref-type="bibr" rid="scirp.64668-ref8">8</xref>]</p><disp-formula id="scirp.64668-formula30"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x18.png"  xlink:type="simple"/></disp-formula><p>That means E(O) is about 4.5% of the maximal energy density of the cosmos, i.e. Einstein’s density while the dark energy density is clearly the self explanatory formula <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x19.png" xlink:type="simple"/></inline-formula> which is nearly 95.5% of Einstein’s maximal energy density E = mc<sup>2</sup> as found in earlier publications and in full agreement with the actual cosmic measurements [<xref ref-type="bibr" rid="scirp.64668-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref7">7</xref>] . Our next task is to give the details of the analysis leading to the preceding result using the suggested methodology of E-infinity theory [<xref ref-type="bibr" rid="scirp.64668-ref6">6</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref11">11</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref19">19</xref>] .</p></sec><sec id="s2"><title>2. The Making of Davis M<sup>(4)</sup> Hyperbolic 4D Manifold with c = 26 to a Transfinite Hyperbolic Manifold with c = 26 + k</title><p>M.W. Davis found in [<xref ref-type="bibr" rid="scirp.64668-ref4">4</xref>] a compact hyperbolic 4-manifold built upon 120-cell PCH<sup>(4)</sup> where P can be cut into 14,400 congruent orthoschemes, each with a volume equal to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x20.png" xlink:type="simple"/></inline-formula>. Consequently we have the total hyperbolic volume [<xref ref-type="bibr" rid="scirp.64668-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref4">4</xref>]</p><disp-formula id="scirp.64668-formula31"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x21.png"  xlink:type="simple"/></disp-formula><p>Now the transfinite harmonization methods of E-infinity theory [<xref ref-type="bibr" rid="scirp.64668-ref6">6</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref9">9</xref>] suggest immediately upon inspecting</p><p>the above expression that 104 should be replaced by 104.7213596, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x22.png" xlink:type="simple"/></inline-formula>by 10 and 3 by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x23.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x24.png" xlink:type="simple"/></inline-formula> is ‘tHooft’s renormalon [<xref ref-type="bibr" rid="scirp.64668-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref15">15</xref>] which is twice the value of Hardy’s entangleon <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x25.png" xlink:type="simple"/></inline-formula></p><p>[<xref ref-type="bibr" rid="scirp.64668-ref12">12</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref20">20</xref>] . Now for the reader not familiar with E-infinity transfinite correction, the simplest thing to make the above plausible is to compute the expression of equation 4 first explicitly [<xref ref-type="bibr" rid="scirp.64668-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref4">4</xref>]</p><disp-formula id="scirp.64668-formula32"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x26.png"  xlink:type="simple"/></disp-formula><p>Subsequently alone from the magnitude of the integer value 342 we notice that (342)(2) = 684 which is almost the value of the sum of all the dimensions of the two and three Stein spaces, namely [<xref ref-type="bibr" rid="scirp.64668-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref18">18</xref>]</p><disp-formula id="scirp.64668-formula33"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x27.png"  xlink:type="simple"/></disp-formula><p>This result in turn is shown in E-infinity theory to be related to the theoretical exact value of the inverse electromagnetic fine structure constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x28.png" xlink:type="simple"/></inline-formula> by [<xref ref-type="bibr" rid="scirp.64668-ref12">12</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref14">14</xref>]</p><disp-formula id="scirp.64668-formula34"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x29.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x30.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x31.png" xlink:type="simple"/></inline-formula> is Hardy’s quantum entangleon [<xref ref-type="bibr" rid="scirp.64668-ref11">11</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref21">21</xref>] . Thus the exact transfinite value for M<sup>(4)</sup> could be surmised from the above to be</p><disp-formula id="scirp.64668-formula35"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x32.png"  xlink:type="simple"/></disp-formula><p>as we concluded earlier on. Confining ourselves to the integer theory only, it is easily reasoned that the 342.7 is approximately equal to 343 the hyperbolic volume of our manifold could be seen as the dimensions of a Klein modular space with its well known 336 degrees of freedom when we add to it the 7 embedding dimension of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x33.png" xlink:type="simple"/></inline-formula> and it becomes 336 + 7 = 343 [<xref ref-type="bibr" rid="scirp.64668-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref9">9</xref>] . Now we can see another novel interpretation of Vol<sub>H</sub>(exact) of M<sup>(4)</sup>, namely by extracting the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x34.png" xlink:type="simple"/></inline-formula> embedding it becomes [<xref ref-type="bibr" rid="scirp.64668-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref15">15</xref>] :</p><disp-formula id="scirp.64668-formula36"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x35.png"  xlink:type="simple"/></disp-formula><p>which is simply equal to the compactified fractal degrees of freedom of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x36.png" xlink:type="simple"/></inline-formula> with a transfinite number of isometries equal to [<xref ref-type="bibr" rid="scirp.64668-ref12">12</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref14">14</xref>]</p><disp-formula id="scirp.64668-formula37"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x37.png"  xlink:type="simple"/></disp-formula><p>where 336 may be seen as say the dim SL(2,7) or R<sup>(8)</sup> of Riemannian tensor in super space D = 8 or alternatively the number of kissing spheres <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x38.png" xlink:type="simple"/></inline-formula> in ten dimensions. In our case we take 338.8854382 as being the</p><p>compactified holographic boundary of our actual spacetime which in an integer approximation of the standard model amounts to 336 plus |SU(2)| = 3 giving us the well known 339. Recalling that the first massless level in Heterotic string theory [<xref ref-type="bibr" rid="scirp.64668-ref16">16</xref>] is given by 8064 and that this may be found either from the bulk or alternatively from the holographic boundary by a multiplication of the degree of freedom of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x39.png" xlink:type="simple"/></inline-formula> and the instanton number n = 24 [<xref ref-type="bibr" rid="scirp.64668-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref12">12</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref16">16</xref>] leading to N<sub>o</sub> = (336)(24) = 8064 then knowing that the exact transfinite number corresponding to 8064 is, in E-infinity, equal to N<sub>o</sub> = (336 + 16k)(24 + 2 + k) = 8872.135957 [<xref ref-type="bibr" rid="scirp.64668-ref9">9</xref>] . From this relation and remembering that c = n for the fuzzy K&#228;hler modelling E-infinity spacetime and taking all the previous results on board, it follows then that the transfinitely corrected M<sup>(4)</sup> will also have the Euler characteristic c = 26 + k rather than c = 26 [<xref ref-type="bibr" rid="scirp.64668-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref4">4</xref>] . In other words the transfinite version of M<sup>(4)</sup> is a fuzzy manifold in the sense of E-infinity theory and consequently E-infinity fuzziness makes the theory more accurate through subjecting our manifold to the same rules of homology and co-homology which we used for our E-infinity K&#228;hler manifold.</p><p>Consequently by squaring <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x40.png" xlink:type="simple"/></inline-formula> one finds</p><disp-formula id="scirp.64668-formula38"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x41.png"  xlink:type="simple"/></disp-formula><p>From the above we see that we are back to the same holographic boundary of our theory and that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x42.png" xlink:type="simple"/></inline-formula> represents an important Betti number of our manifold of cohomology [<xref ref-type="bibr" rid="scirp.64668-ref6">6</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref16">16</xref>] while <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x43.png" xlink:type="simple"/></inline-formula> is basically</p><p>the Immirzi parameter of our analysis which may be interpreted as the entanglement probability of two self entangled points in our space, each with self entanglement probability<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x44.png" xlink:type="simple"/></inline-formula>. This is the inverse of the expectation value of the Hausdorff dimensions of E-infinity spacetime, i.e. [<xref ref-type="bibr" rid="scirp.64668-ref9">9</xref>]</p><disp-formula id="scirp.64668-formula39"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x45.png"  xlink:type="simple"/></disp-formula><p>This way we see that our analysis is circulatory consistent.</p></sec><sec id="s3"><title>3. The Energy Density of Our Cosmos</title><p>Now we are in a position to tackle the task of determining the energy density of ordinary energy and consequently that of dark energy of the cosmos. Using the so far obtained insight into the “fuzzy” or transfinite M<sup>4</sup> it is not difficult to reason that the maximal E of Einstein density was based on 4D space. That would mean that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x46.png" xlink:type="simple"/></inline-formula>degrees of freedom of the theory were not considered in relation to 336 + 16k minus 16</p><p>of the holographic boundary of our theory. Since E = mc<sup>2</sup> is the maximal one hundred percent energy density, then writing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x47.png" xlink:type="simple"/></inline-formula> means that E<sub>max</sub> is given by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x48.png" xlink:type="simple"/></inline-formula>. We may stress at this point that looking at E = mc<sup>2</sup> as the maximal energy density possible in the cosmos is a crucial point in our theory and deceptively simple and is far from being trivial. On the other hand assuming that E-infinity spacetime and consequently M<sup>4</sup> is our real spacetime, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x49.png" xlink:type="simple"/></inline-formula> should not be <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x50.png" xlink:type="simple"/></inline-formula> but [<xref ref-type="bibr" rid="scirp.64668-ref8">8</xref>]</p><disp-formula id="scirp.64668-formula40"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x51.png"  xlink:type="simple"/></disp-formula><p>Consequently we have to expect the measured ordinary energy density to be [<xref ref-type="bibr" rid="scirp.64668-ref11">11</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref15">15</xref>]</p><disp-formula id="scirp.64668-formula41"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x52.png"  xlink:type="simple"/></disp-formula><p>This then implies a “missing” dark energy density of</p><disp-formula id="scirp.64668-formula42"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x53.png"  xlink:type="simple"/></disp-formula><p>Setting k @ 0, this simplifies to our previously obtained results [<xref ref-type="bibr" rid="scirp.64668-ref11">11</xref>] - [<xref ref-type="bibr" rid="scirp.64668-ref15">15</xref>]</p><disp-formula id="scirp.64668-formula43"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x54.png"  xlink:type="simple"/></disp-formula><p>Note here, as elsewhere, how k plays a crucial role in smoothing the analyses and easing the reaching of general conclusions and deeper insight. In a manner of speech we could say that we put the entire problem under a transfinite microscope enabling us to see how ‘tHooft’s renormalon hypothetical elementary particle works [<xref ref-type="bibr" rid="scirp.64668-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref15">15</xref>] . This normalon is actually made of two other hypothetical particles, namely Hardy’s entangleon <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-8302729x55.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.64668-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.64668-ref8">8</xref>] since</p><disp-formula id="scirp.64668-formula44"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-8302729x56.png"  xlink:type="simple"/></disp-formula><p>Pondering this situation we see that the real power of transfinite correction is the following: while overwhelmingly integer based theories are to a far extent consistent, we notice that we have many different theories leading to similar results although they differ substantially from each other at various stages. Transfinite correction fuses different theories and shows that they are exactly the same and that everything fits with everything else at all stages of the analysis. We will address the same subject at various occasions in the rest of the present paper.</p></sec>
<sec id="s4">
<title>4. Transfiniteness―A View from the Standard Model</title>
<p>Seen in the conventional way the standard model contains twelve messenger particles given by the symmetry breaking ofSU(3) SU(2) U(1) dimensions. The experimental discovery of the Higgs is not included in the above, nor is the not discovered yet graviton let alone all super symmetric partners. However seen under the transfinite microscope, E-infinity theory tells us something quite if not radically different. The reason for this deviation is that E-infinity extends fuzziness, i.e. transfiniteness to the counting of particles. It is ordinary counting but with a fractal-Cantorian weight linked to it. This so called fractal logic of counting particles mutates the standard model to a truly magical structure by the following transformation from integer to transfinite counting were we will write on the left hand side the classical counting vis-&#224;-vis the transfinite weight counting on the right hand side of the following <xref ref-type="table" rid="table1">Table 1</xref> [<xref ref-type="bibr" rid="scirp.64668-ref17">17</xref>] .</p></sec></body>
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